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Author SHA1 Message Date
9e3ee37ecf idk 2025-03-06 08:53:34 -05:00
fd13c627c1 ME2046 hw3 prayers pls 2025-02-27 13:57:14 -05:00
579e7cd0aa NUCE 2113 lab 5 2025-02-24 16:12:02 -05:00
21 changed files with 7563 additions and 0 deletions

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ME_2046/HW3/simplifying.py Normal file
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import sympy as sm
import numpy as np
sm.init_printing()
s = sm.symbols('s')
z = sm.symbols('z')
T = sm.symbols('T')
#########################################################
print('PROBLEM 2:')
print('Part a:')
ZOH = (1-sm.exp(-s*T))/(s*T)
G_1_s = 1/s*ZOH
bilinear_s = 2/T *(z-1)/(z+1)
G_1_k = G_1_s.subs({s:bilinear_s}).simplify()
print("G_1_k = ")
sm.pprint(G_1_k)
print('Part b:')
theta_s_r_s = ZOH*1/s**2
theta_k_r_k = theta_s_r_s.subs({s:bilinear_s}).simplify()
print("theta_k_r_k = ")
sm.pprint(theta_k_r_k)
#########################################################
print('PROBLEM 3:')
A = sm.Matrix([[0, 1, 0, 0],
[0, 0, 1, 0],
[0, 0, 0, 1],
[1, 0, 0, 0]])
B = sm.Matrix([0, 0, 0, 1])
C = sm.Matrix([1, 0, 0, 0]).transpose()
D = sm.Matrix([1])
print('System Matricies A, B, C, D')
sm.pprint(A)
sm.pprint(B)
sm.pprint(C)
sm.pprint(D)
#Recursive Solution
k = sm.symbols('k', integer = True, real = True, positive = True)
def y(k,u):
term_1 = C * A**k * x_0
term_2 = sm.Matrix([0,0,0,0])
for j in range(np.size(u)):
term_2 = term_2 + A**(k-j-1) * B * u[j]
term_2 = C*term_2
term_3 = D*u[-1]
return term_1+term_2+term_3
print('Part c:')
x_0 = sm.Matrix([2, 1, 3, 0])
u = sm.Matrix([0])
output = y(k, u)
output = output[0].expand().simplify()
print('y(k) = ')
sm.pprint(output)
print('Part d:')
x_0 = sm.Matrix([0, 0, 0, 0])
u = sm.Matrix([2, 1, 3, 0])
output = y(k, u)
output = output[0].expand().simplify()
print('y(k) = ')
sm.pprint(output)
print('Part e:')
print('These are the same exact response between parts C and D. This makes sense, becasue we defined our states as just being delays in a chain. The result is that the input at timestep k trickles down through each state in k+1, k+2, and k+3. This means that our states save our input in a way, s.t. loading this initial state mathematically produces an identical result as loading those inputs in one time step at a time. \n \n This is reflected by the two algebraeic expressions being the same.')
#########################################################
print('PROBLEM 4:')
print('Part a:')
"""
x(k+2) - x(k+1) + 0.25 x(k) = u(k+2)
Applying Z transform:
z^2 X - z X + 0.25 X = z^2 U
X (z^2 - z + 0.25) = z^2 U
X/U = z^2 / (z^2 - z + 0.25)
"""
# Use SymPy to do partial frac
z = sm.symbols('z')
X_U = z**2/(z**2 - z + 0.25)
sm.pprint(X_U.apart())

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NUCE_2113/lab5/labviz.ods Normal file

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NUCE_2113/lab5/viz.py Normal file
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import glob
import os
import numpy as np
import matplotlib.pyplot as plt
def load_spectrum_data(filename):
"""
Load spectrum data from a text file in the provided format.
This function:
- Reads the file line by line.
- Finds the "$DATA:" section.
- Skips the first line after "$DATA:" (assumed to be the channel range header).
- Collects all subsequent lines (until the next section indicated by a line starting with '$').
- Parses these lines into a NumPy array.
Parameters:
filename (str): Path to the spectrum file.
Returns:
numpy.ndarray: Array of count values.
"""
with open(filename, 'r') as f:
lines = f.readlines()
data_lines = []
in_data_section = False
skip_first_data_line = True # flag to skip the channel-range header
for line in lines:
# Look for the beginning of the data section
if line.strip().startswith("$DATA:"):
in_data_section = True
continue
if in_data_section:
# If we hit a new section header, exit the data section
if line.strip().startswith("$"):
break
# Skip the first line after "$DATA:" if it contains exactly two numbers (channel range header)
if skip_first_data_line:
parts = line.strip().split()
if len(parts) == 2:
skip_first_data_line = False
continue
skip_first_data_line = False # even if not two numbers, do not skip subsequent lines
# Append non-empty lines
if line.strip():
data_lines.append(line.strip())
# Combine the collected lines into one string and parse numbers
data_str = " ".join(data_lines)
# Convert the string of numbers into a NumPy array
data = np.fromstring(data_str, sep=' ')
return data
# Get a list of all .Spe files in the current directory
spe_files = glob.glob("*.Spe")
# To store data for the combined plot
combined_data = []
for file in spe_files:
# Load the spectrum data
spectrum_data = load_spectrum_data(file)
# Create an array for channel numbers (one per data point)
channels = np.arange(len(spectrum_data))
# Store the data for the combined plot (use file name without extension for legend)
base_name = os.path.splitext(os.path.basename(file))[0]
combined_data.append((base_name, channels, spectrum_data))
# Plot individual spectrum
plt.figure(figsize=(10, 6))
plt.step(channels, spectrum_data, where='mid', color='blue')
plt.xlabel('Channel')
plt.ylabel('Counts')
plt.title(f"Spectrum: {base_name}")
plt.grid(True)
plt.tight_layout()
# Save individual figure as PNG
output_filename = base_name + '.png'
plt.savefig(output_filename)
plt.close() # Close the figure to free memory
# Now create a combined plot with all spectra
plt.figure(figsize=(12, 8))
for name, channels, spectrum_data in combined_data:
# Do not specify a color so that the default cycle gives different colors for each curve
plt.step(channels, spectrum_data, where='mid', label=name)
plt.xlabel('Channel')
plt.ylabel('Counts')
plt.title("Combined Spectrum Data")
plt.grid(True)
plt.legend()
plt.tight_layout()
# Save and display the combined plot
plt.savefig('combined_spectrum.png')
plt.show()

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NUCE_2113/lab5/viz2.py Normal file
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